Supernova Remnants As Clues to Their Progenitors

Total Page:16

File Type:pdf, Size:1020Kb

Supernova Remnants As Clues to Their Progenitors Supernova Remnants as Clues to Their Progenitors Daniel Patnaude and Carles Badenes Abstract Supernovae shape the interstellar medium, chemically enrich their host galaxies, and generate powerful interstellar shocks that drive future generations of star formation. The shock produced by a supernova event acts as a type of time ma- chine, probing the mass loss history of the progenitor system back to ages of ∼ 10 000 years before the explosion, whereas supernova remnants probe a much earlier stage of stellar evolution, interacting with material expelled during the progenitor’s much earlier evolution. In this chapter we will review how observations of super- nova remnants allow us to infer fundamental properties of the progenitor system. We will provide detailed examples of how bulk characteristics of a remnant, such as its chemical composition and dynamics, allow us to infer properties of the progeni- tor evolution. In the latter half of this chapter, we will show how this exercise may be extended from individual objects to SNR as classes of objects, and how there are clear bifurcations in the dynamics and spectral characteristics of core collapse and thermonuclear supernova remnants. We will finish the chapter by touching on re- cent advances in the modeling of massive stars, and the implications for observable properties of supernovae and their remnants. 1 Introduction Supernova remnants provide a unique view of the supernova (SN) phenomenon. The hundreds of extragalactic supernovae (SNe) discovered each year by modern Daniel Patnaude Smithsonian Astrophysical Observatory, 60 Garden St, Cambridge, MA 02138, e-mail: arXiv:1702.03228v1 [astro-ph.HE] 10 Feb 2017 [email protected] Carles Badenes Department of Physics and Astronomy, and Pittsburgh Particle Physics, Astrophysics, and Cosmol- ogy Center (PITT-PACC), University of Pittsburgh, 3931 O’Hara St, Pittsburgh, PA 15260 e-mail: [email protected] 1 2 Daniel Patnaude and Carles Badenes surveys are unresolved point sources which fade before they can interact with any circumstellar material outside of their most immediate surroundings. Before they fade, they probe the evolution of the progenitor on timescales of ∼ 100–1000 years before the explosion. This is because the typical outflow speeds from the progenitor are ∼ 10–1000 km s−1, 100-1000× slower than the typical supernova blastwave velocity. In contrast, supernova remnants (SNRs) in the Local Group galaxies can be re- solved in some detail as they interact with the bulk of the circumstellar material expelled by their progenitors during pre-SN mass loss over much longer timescales. Additionally, SNRs are surrounded by resolved stellar populations that spawned their SN progenitors (Badenes et al., 2009; Williams et al., 2014; Jennings et al., 2014), and they have become prime hunting grounds in the search for their surviv- ing binary companions (e.g., Edwards et al., 2012; Kerzendorf et al., 2014). X-ray spectra of SNRs can reveal emission from neutron-rich isotopes in the ejecta which are sensitive probes of SN explosion mechanisms (e.g., Yamaguchi et al., 2015). In short, SNR observations can constrain aspects of SNe and their progenitors that are either difficult or impossible to access by optical SN observations. In this chapter, we review the clues that supernova remnants provide about their progenitor’s evolution and ultimate fate. We begin by highlighting studies of both Type Ia and core-collapse SNRs which inferred properties of their progenitors and evolution. We then discuss recent techniques that use bulk SNR observables to con- strain SN progenitor properties. We conclude by touching on recent results in mas- sive star evolution which may be relevant towards understanding observable prop- erties in supernova remnants. For further background and a different perspective of these topics, see the reviews by Badenes (2010) and Vink (2012). 2 Supernova Remnant - Progenitor Connections The main challenge associated with studying supernova remnants is related to their type. Classically, SNe have been typed by their optical spectrum around maximum light (Filippenko, 1997). In general terms, Type Ia supernovae show no hydrogen in their optical spectra, with Type Ia (thermonuclear) SNe exhibiting strong Si II absorption around 615 nm. Type Ib/c are core-collapse supernovae, and differ from Ia SNe in that they possess either a weak or non-existent silicon absorption feature, and little (Type Ib) or no (Ic) absorption from He I. The amount of helium in the optical spectrum may provide insight into the degree of mass-loss in the progenitor prior to core-collapse. In contrast, Type II SNe do show hydrogen in their spectra, and are further subdivided into types IIP, IIL, IIb and IIn, based on the evolution and characteristics of their light curve or, in the case of Type IIn SNe, their optical spectrum. While SNe are common and somewhat accessible to typing, SNRs are evolved objects, and a priori it is non-trivial to associate them with each of the established SN types, though the detection of optical light echoes from the SN event do provide Supernova Remnants as Clues to Their Progenitors 3 clues in some cases (Rest et al., 2008). However, given the wealth of data available, a challenging opportunity exists to connect remnant properties back to the properties of the progenitor. Connecting remnant properties to those of the progenitor often involves a detailed analysis of the remnant’s broadband spectrum, combined with comparisons to hy- drodynamical models for supernova remnant ejecta evolution. In some cases such as those discussed below, this has produced interesting constraints. However, bulk properties such as emission line strengths, energy centroids, and chemical abun- dances depend on different aspects of a SN explosion than those of optical SNe. These properties can act as crucial benchmarks for specific stellar evolution sce- narios. In x 3 of this chapter, we explore how these so called “bulk observables” connect directly to the evolution of the progenitor, and how theorists and observers are connecting detailed stellar evolution models to properties of young supernova remnants. When studying SNRs, both as individual objects and as a class, the main proper- ties to consider are the chemical composition of the ejecta and the dynamics of the blast wave. The spectrum of a SNR in the X-ray band is a combination of nonthermal emission from the blast wave, and thermal emission from both swept-up circumstel- lar material and shocked supernova ejecta. The chemical composition of the shocked ejecta is determined by fitting models to the observed X-ray spectrum, which often requires some knowledge of the SNR dynamics (Borkowski et al., 2001). In turn, the blast wave dynamics are inferred by relying on critical assumptions about the re- lationship between the shock speed and the measured electron temperature. Only in certain cases, such as in the Galactic SNR Cas A, are the dynamics directly observed (DeLaney & Rudnick, 2003; Patnaude & Fesen, 2009). In most cases, the morphology is compared to self-similar models for blast wave evolution, which again require assumptions about the remant’s age, energetics, and circumstellar environment. These methods are vulnerable to circular logic and can result in detailed statements about the properties of a given SNR that fail to properly account for the considerable uncertainties introduced by the models. In other words, the critical assumptions made in connecting spectral properties to dynamics often compromise the the connections made back to the progenitor evolution. As an example, specific stellar evolution scenarios from SN Ia progenitors pre- dict circumstellar structures that range from the r ∝ r−2 profiles that are the sig- nature of isotropic mass-loss to relatively large low-density energy-driven cavities excavated by fast outflows from accreting white dwarfs (Badenes et al., 2007; Shen et al., 2013). As seen in Figure 1, the prompt radio and X-ray emission from SNe (Chomiuk et al., 2016; Margutti et al., 2014), weeks or months after the explosion, can only probe circumstellar material (CSM) structures up to a few hundred AU, composed of material expelled by the progenitor hundreds to thousands of years before the explosion, depending on the outflow velocity. In contrast, SNRs that are hundreds or thousands of years old can probe CSM structures up to several pc in size, expelled by the progenitor several thousands to millions of years before the explosion. These spatial scales are representative of typical stellar wind blown bubbles (Koo & McKee, 1992), and the associated 4 Daniel Patnaude and Carles Badenes temporal scales are directly relevant to stellar evolution scenarios for Type Ia SN progenitors (Wang & Han, 2012). For CC SNRs, the argument is even stronger, as mass-loss is often the single most uncertain ingredient in stellar evolution models for SN progenitors (Smith, 2014). Fig. 1 Schematic circumstellar density profiles for isotropic SN Ia progenitor outflows (colored −1 3 −1 plots, dashed for uw = 20 km s ; solid for uw = 10 km s ), compared to the typical densities in the warm phase of the interstellar medium (horizontal grey band) (Ferriere,` 2001). The rulers on top of the plots show the time before the explosion (in yr) when the material at that radius was ejected by the SN progenitor. The rulers on the bottom show the typical sizes of circumstellar cavities excavated by fast outflows (Badenes et al., 2007; Shen et al., 2013). The radii probed by X-ray/radio follow-up observations of SNe and studies of Type Ia SNRs are shown by blue and red shaded vertical stripes. The blue arrows and red circles show upper limits for two Type Ia SNe (Chomiuk et al., 2016; Perez-Torres´ et al., 2014) and measurements for three Type Ia SNRs (Raymond et al., 2007; Slane et al., 2014; Borkowski et al., 2014). A different approach is instead of studying the minute details of individual ob- jects, one probes the general characteristics of SNRs to see how they relate to the expected characteristics of a model derived from a potential progenitor scenario.
Recommended publications
  • Supernovae Sparked by Dark Matter in White Dwarfs
    Supernovae Sparked By Dark Matter in White Dwarfs Javier F. Acevedog and Joseph Bramanteg;y gThe Arthur B. McDonald Canadian Astroparticle Physics Research Institute, Department of Physics, Engineering Physics, and Astronomy, Queen's University, Kingston, Ontario, K7L 2S8, Canada yPerimeter Institute for Theoretical Physics, Waterloo, Ontario, N2L 2Y5, Canada November 27, 2019 Abstract It was recently demonstrated that asymmetric dark matter can ignite supernovae by collecting and collapsing inside lone sub-Chandrasekhar mass white dwarfs, and that this may be the cause of Type Ia supernovae. A ball of asymmetric dark matter accumulated inside a white dwarf and collapsing under its own weight, sheds enough gravitational potential energy through scattering with nuclei, to spark the fusion reactions that precede a Type Ia supernova explosion. In this article we elaborate on this mechanism and use it to place new bounds on interactions between nucleons 6 16 and asymmetric dark matter for masses mX = 10 − 10 GeV. Interestingly, we find that for dark matter more massive than 1011 GeV, Type Ia supernova ignition can proceed through the Hawking evaporation of a small black hole formed by the collapsed dark matter. We also identify how a cold white dwarf's Coulomb crystal structure substantially suppresses dark matter-nuclear scattering at low momentum transfers, which is crucial for calculating the time it takes dark matter to form a black hole. Higgs and vector portal dark matter models that ignite Type Ia supernovae are explored. arXiv:1904.11993v3 [hep-ph] 26 Nov 2019 Contents 1 Introduction 2 2 Dark matter capture, thermalization and collapse in white dwarfs 4 2.1 Dark matter capture .
    [Show full text]
  • Formation of Dust and Molecules in Supernovae
    2019/02/06 Formation of dust and molecules in supernovae Takaya Nozawa (National Astronomical Observatory of Japan) SN 1987A Cassiopeia A SNR 0509-67.5 1-1. Introduction Question : Can supernovae (SNe) produce molecules and dust grains? Nozawa 2014, Astronomical Herald 2-1. Thermal emission from dust in SN 1987A light curve 60day 200day (optical luminosity) 415day 615day Whitelock+89 - dust starts to form in the 755day ejecta at ~400 days - dust mass ay 775 day: > ~10-4 Msun (optically thin assumed) Wooden+93 2-2. CO and SiO detection in SN 1987A CO first overtone: 2.29-2.5 μm 97 day CO fundamental: 4.65-6.0 μm SiO fundamental: 7.6-9.5 μm 200day SN Ic 2000ew, Gerardy+2002 415day 615day 58 day 755day SN II-pec 1987A, Wooden+1993 SN II-P 2016adj, Banerjee+2018 2-3. CO and SiO masses in SN 1987A CO Gerardy+2002, see also Banerjee+2018 Liu+95 ‐CO emission is seen in various SiO types of CCSNe from ~50 day ‐CO/SiO masses in SN 1987A Mco > ~4x10-3 Msun MSiO > ~7x10-4 Msun Liu & Dalgarno 1996 2-4. Dust mass in Cassiopeia A (Cas A) SNR ○ Estimated mass of dust in Cas A ・ warm/hot dust (80-300K) (3-7)x10-3 Msun (IRAS, Dwek et al. 1987) ~7.7x10-5 Msun (ISO, Arendt et al. 1999) 0.02-0.054 Msun (Spitzer, Rho+2008) ➜ Mdust = 10-4-10-2 Msun consistent with >10-4 Msun in SN 1987A Dwek+1987, IRAS Rho+2008 Spitzer Arendt+1999, ISO 3-1.
    [Show full text]
  • How Supernovae Became the Basis of Observational Cosmology
    Journal of Astronomical History and Heritage, 19(2), 203–215 (2016). HOW SUPERNOVAE BECAME THE BASIS OF OBSERVATIONAL COSMOLOGY Maria Victorovna Pruzhinskaya Laboratoire de Physique Corpusculaire, Université Clermont Auvergne, Université Blaise Pascal, CNRS/IN2P3, Clermont-Ferrand, France; and Sternberg Astronomical Institute of Lomonosov Moscow State University, 119991, Moscow, Universitetsky prospect 13, Russia. Email: [email protected] and Sergey Mikhailovich Lisakov Laboratoire Lagrange, UMR7293, Université Nice Sophia-Antipolis, Observatoire de la Côte d’Azur, Boulevard de l'Observatoire, CS 34229, Nice, France. Email: [email protected] Abstract: This paper is dedicated to the discovery of one of the most important relationships in supernova cosmology—the relation between the peak luminosity of Type Ia supernovae and their luminosity decline rate after maximum light. The history of this relationship is quite long and interesting. The relationship was independently discovered by the American statistician and astronomer Bert Woodard Rust and the Soviet astronomer Yury Pavlovich Pskovskii in the 1970s. Using a limited sample of Type I supernovae they were able to show that the brighter the supernova is, the slower its luminosity declines after maximum. Only with the appearance of CCD cameras could Mark Phillips re-inspect this relationship on a new level of accuracy using a better sample of supernovae. His investigations confirmed the idea proposed earlier by Rust and Pskovskii. Keywords: supernovae, Pskovskii, Rust 1 INTRODUCTION However, from the moment that Albert Einstein (1879–1955; Whittaker, 1955) introduced into the In 1998–1999 astronomers discovered the accel- equations of the General Theory of Relativity a erating expansion of the Universe through the cosmological constant until the discovery of the observations of very far standard candles (for accelerating expansion of the Universe, nearly a review see Lipunov and Chernin, 2012).
    [Show full text]
  • Elliptical Galaxies Where Star Formation Is Thought to Have Ceased Long Ago → the Star That Explodes Is Old, Billions of Years
    Monday, February 3, 2014 First Exam, Skywatch, Friday February 7. Review sheet posted today. Review session Thursday, 5 – 6 PM, RLM 7.104 Reading: Section 5.1 (white dwarfs), 1.2.4 (quantum theory), Section 2.3 (quantum deregulation), Section 6.1 (supernovae; not Type Ib, Type Ic, next exam). Astronomy in the news? Update on new “nearby” supernova SN 2014J in M82 Our second attempt to measure the shape of the explosion with a telescope at Calar Alto, Spain, was messed up by weather. We are attempting to schedule time on MONET, a newly-robotocized telescope at McDonald Observatory, operated by collaborators in Germany. First spectrum Sulfur from Hubble Space Telescope Intensity Silicon Calcium Magnesium Wavelength Goal: To understand the observed nature of supernovae and determine whether they came from white dwarfs or massive stars that undergo core collapse. Categories of Supernovae 1st category discovered Type Ia – near peak light, no detectable Hydrogen or Helium in the spectrum, rather “intermediate mass elements” such as oxygen, magnesium, silicon, sulfur, calcium. Iron appears later as the light fades. Type Ia occur in all galaxy types: In spiral galaxies they tend to avoid the spiral arms, they have had time to drift away from the birth site → the star that explodes is old In elliptical galaxies where star formation is thought to have ceased long ago → the star that explodes is old, billions of years" the progenitor that explodes must be long-lived, not very massive, suggesting a white dwarf. Sun is long-lived, but won’t explode weeks Type Ia - no hydrogen or helium, Luminosity intermediate mass elements early, iron later SN 2014J about here Light Curve - brightness vs.
    [Show full text]
  • Science from the Mev Gamma Ray Sky
    Science from the MeV Gamma Ray Sky Reshmi Mukherjee Barnard College, Columbia University, NY Reshmi Mukherjee The need …. - A sensitive survey of the γ-ray sky between 100 keV and 100 MeV 10-9 10-10 10-12 10-14 10-16 10-18 10-20 m 100 keV 0.5 MeV 100 TeV Reshmi Mukherjee Energy range & challenges . Energy range 300 keV to ~100 MeV . “Compton regime” -- notoriously difficult & challenging . Requires an efficient instrument with an excellent background subtraction . Last instrument to operate in this range: COMPTEL . Neither Fermi-LAT nor AGILE are optimized for observations below ~200 MeV or for polarization sensitivity. Freytag, Handbook of Accel. Phys. & Eng. (1971) Reshmi Mukherjee Compton Imaging McConnell, AAS 225th Reshmi Mukherjee Sensitivities - The MeV “Gap” / VERITAS From Takahashi 2012 Reshmi Mukherjee Talk Outline . Science motivation . Review highlights from “MeV” missions . Synergy with VHE and keV regime . Wish list for a future medium-energy instrument Reshmi Mukherjee Science goals for the “medium energy” . Explosive nucleosynthesis : a close look at core-collapse and thermonuclear supernovae . γ-ray lines (e.g. 511 keV, 70 MeV, + + + ) . Large number of soft γ-ray sources in the Galactic plane, yet to be discovered . Contribution of soft γ-ray sources to the medium-energy Galactic diffuse emission . The laws of physics around neutron stars and black holes . Measurements of transient phenomena . Spatially resolve variation between electron dominated and hadron dominated processes in the 70-200 MeV range.. Origin of cosmic rays? Reshmi Mukherjee from AstroMeV Origin of the highest energy cosmic rays? . >100 year old mystery ! . Enormous E range .
    [Show full text]
  • Asymmetries in Sn 2014J Near Maximum Light Revealed Through Spectropolarimetry
    ASYMMETRIES IN SN 2014J NEAR MAXIMUM LIGHT REVEALED THROUGH SPECTROPOLARIMETRY Item Type Article Authors Porter, Amber; Leising, Mark D.; Williams, G. Grant; Milne, P. A.; Smith, Paul; Smith, Nathan; Bilinski, Christopher; Hoffman, Jennifer L.; Huk, Leah; Leonard, Douglas C. Citation ASYMMETRIES IN SN 2014J NEAR MAXIMUM LIGHT REVEALED THROUGH SPECTROPOLARIMETRY 2016, 828 (1):24 The Astrophysical Journal DOI 10.3847/0004-637X/828/1/24 Publisher IOP PUBLISHING LTD Journal The Astrophysical Journal Rights © 2016. The American Astronomical Society. All rights reserved. Download date 27/09/2021 22:28:24 Item License http://rightsstatements.org/vocab/InC/1.0/ Version Final published version Link to Item http://hdl.handle.net/10150/622057 The Astrophysical Journal, 828:24 (12pp), 2016 September 1 doi:10.3847/0004-637X/828/1/24 © 2016. The American Astronomical Society. All rights reserved. ASYMMETRIES IN SN 2014J NEAR MAXIMUM LIGHT REVEALED THROUGH SPECTROPOLARIMETRY Amber L. Porter1, Mark D. Leising1, G. Grant Williams2,3, Peter Milne2, Paul Smith2, Nathan Smith2, Christopher Bilinski2, Jennifer L. Hoffman4, Leah Huk4, and Douglas C. Leonard5 1 Department of Physics and Astronomy, Clemson University, 118 Kinard Laboratory, Clemson, SC 29634, USA; [email protected] 2 Steward Observatory, University of Arizona, 933 N. Cherry Avenue, Tucson, AZ 85721, USA 3 MMT Observatory, P.O. Box 210065, University of Arizona, Tucson, AZ 85721-0065, USA 4 Department of Physics and Astronomy, University of Denver, 2112 East Wesley Avenue, Denver, CO 80208, USA 5 Department of Astronomy, San Diego State University, PA-210, 5500 Campanile Drive, San Diego, CA 92182-1221, USA Received 2016 February 14; revised 2016 May 11; accepted 2016 May 12; published 2016 August 24 ABSTRACT We present spectropolarimetric observations of the nearby Type Ia supernova SN 2014J in M82 over six epochs: +0, +7, +23, +51, +77, +109, and +111 days with respect to B-band maximum.
    [Show full text]
  • Posters for Presentation at Gamma2016 (As of 01.07.2016) 1
    Posters for presentation at Gamma2016 (as of 01.07.2016) 1. Adamczyk, Katarzyna: Cloud transmission and its impact on the Cherenkov light density! 2. Ambrogi, Lucia: On the potential of atmospheric Cherenkov telescope arrays to perform spectral studies of TeV gamma-ray sources! 3. Angioni, Roberto: VLBI and gamma-ray studies of TANAMI radio galaxies! 4. Anguner, Ekrem Oguzhan: HESS J1826-130: a very hard-spectrum gamma-ray source in the Galactic plane! 5. Anjos, Rita: Gamma rays and magnetic fields as a probe for UHECR luminosity! 6. Araya, Miguel: The GeV counterpart of VER J2019+407 in the shell of the SNR G78.2+2.1! 7. Armstrong, Thomas: Detection of VHE AGN in Fermi-LAT Pass 8 Data Using DBSCAN! 8. Baghmanyan, Vardan: Gamma-ray variability of NGC 1275! 9. Banasinski, Piotr: Dynamical Inhomogeneous Model for High Energy Emission from blazars! 10. Barkov, Maxim: Ultrafast VHE gamma-ray flares of AGN: Challenges and Implications! 11. Becerril, Ana: Triggered Searches of GRBs with HAWC! 12. Bernhard, Sabrina: Sensitivity and performance studies by simulating transient phenomena within the H.E.S.S. analysis framework! 13. Bonnoli, Giacomo: Perspectives on observations of extra-galactic sources and fundamental physics studies with the ASTRI mini-array on the path towards the Cherenkov Telescope Array! 14. Braiding, Catherine: The Mopra Southern Galactic Plane CO Survey! 15. Bretz, Thomas: Design study of air-Cherenkov telescopes for harsh environments with efficient air-shower detection at 100 TeV! 16. Bryan, Mark: RX J1713 with H.E.S.S.II! 17. Burtovoi, Aleksandr: Prospects for PWNe and SNRs science with the ASTRI mini-array of pre-production small-sized telescopes of the Cherenkov Telescope Array! 18.
    [Show full text]
  • What Is the Progenitor of the Type Ia SN 2014J?
    Highlights of Spanish Astrophysics VIII, Proceedings of the XI Scientific Meeting of the Spanish Astronomical Society held on September 8–12, 2014, in Teruel, Spain. A. J. Cenarro, F. Figueras, C. Hernández-Monteagudo, J. Trujillo Bueno, and L. Valdivielso (eds.) What is the progenitor of the Type Ia SN 2014J? M. A. P´erez-Torres1;2, P. Lundqvist3;4, R. J. Beswick5, C. I. Bj¨ornsson3, T.W.B. Muxlow5, Z. Paragi6, S. Ryder7, A. Alberdi1, C. Fransson3;4, J. M. Marcaide8, I. Mart´ı-Vidal9, E. Ros8;10, M. K. Argo5 and J. C. Guirado10;11 1 Instituto de Astrof´ısica de Andaluc´ıa,Glorieta de la Astronom´ıa,s/n, E-18008 Granada, Spain. 2 Centro de Estudios de la F´ı´ısicadel Cosmos de Arag´on,E-44001 Teruel, Spain. 3Department of Astronomy, Stockholm University, SE-10691, Sweden. 4The Oskar Klein Centre, AlbaNova, SE-10691 Stockholm, Sweden. 5Jodrell Bank Centre for Astrophysics, University of Manchester, Oxford Road, Manchester. 6Joint Institute for VLBI in Europe, Postbus 2, 7990 AA Dwingeloo, NL. 7Australian Astronomical Observatory, P.O. Box 915, North Ryde, NSW 1670, Australia. 8Depto. de Astronom´ıai Astrof´ısica,Universidad de Valencia, E-46100 Burjassot, Valencia, Spain. 9Onsala Space Observatory, Chalmers University of Technology, SE-43992 Onsala, Sweden. 10Max-Planck-Institut f¨urRadioastronomie, D-53121 Bonn, Germany. 11Observatorio Astron´omico,Universidad de Valencia, E-46980 Paterna, Valencia, Spain. Abstract We report the deepest radio interferometric observations of the closest Type Ia supernova in decades, SN 2014J, which exploded in the nearby galaxy M 82. These observations represent, together with radio observations of SNe 2011fe, the most sensitive radio studies of a Type Ia SN ever.
    [Show full text]
  • Asymmetric Type-Ia Supernova Origin of W49B As Revealed from Spatially Resolved X-Ray Spectroscopic Study Ping Zhou1,2 and Jacco Vink1,3
    A&A 615, A150 (2018) Astronomy https://doi.org/10.1051/0004-6361/201731583 & © ESO 2018 Astrophysics Asymmetric Type-Ia supernova origin of W49B as revealed from spatially resolved X-ray spectroscopic study Ping Zhou1,2 and Jacco Vink1,3 1 Anton Pannekoek Institute, University of Amsterdam, PO Box 94249, 1090 GE Amsterdam, The Netherlands e-mail: p.zhou,[email protected] 2 School of Astronomy and Space Science, Nanjing University, Nanjing 210023, PR China 3 GRAPPA, University of Amsterdam, PO Box 94249, 1090 GE Amsterdam, The Netherlands Received 17 July 2017 / Accepted 23 March 2018 ABSTRACT The origin of the asymmetric supernova remnant (SNR) W49B has been a matter of debate: is it produced by a rare jet-driven core- collapse (CC) supernova, or by a normal supernova that is strongly shaped by its dense environment? Aiming to uncover the explosion mechanism and origin of the asymmetric, centrally filled X-ray morphology of W49B, we have performed spatially resolved X-ray spectroscopy and a search for potential point sources. We report new candidate point sources inside W49B. The Chandra X-ray spectra from W49B are well-characterized by two-temperature gas components ( 0:27 keV + 0.6–2.2 keV). The hot component gas shows a large temperature gradient from the northeast to the southwest and is over-ionized∼ in most regions with recombination timescales 11 3 of 1–10 10 cm− s. The Fe element shows strong lateral distribution in the SNR east, while the distribution of Si, S, Ar, Ca is relatively× smooth and nearly axially symmetric.
    [Show full text]
  • Supernovae and Supernova Remnants
    Supernovae and supernova remnants Mikako Matsuura (Cardiff University) Why are SNe & SNRs important? Path to the first dust in the Universe • Synthase heavy elements Condensation to dust O • dust formation Fe Si • Source of kinetic energy into the ISM C • dust destruction Injection of elements Supernovae – death of massive stars Formation of the first generation of stars Big Bang Why are SNe & SNRs important? • Synthase heavy elements • dust formation • Source of kinetic energy into the ISM • dust destruction Supernova remnant NGC 6960 (Veil Nebula) 100-1000 km s-1 Shocks M82 Galactic outflow Key questions • Are supernovae & supernova remnants dust producer or destroyer? • If dust producer: • What is the net dust mass? • What types of dust grains are formed? • If destroyer: • How efficient? • How does affect grain size distributions? It is getting clear that SNe form substantial mass of dust using newly synthesized elements Cassiopeia A (AD 1681?) Crab Nebula (AD 1054 ) Supernova 1987A SNe in nearby galaxies 0.1-0.5 M¤ 0.03-0.05 M¤ ~0.5 M¤ 0.0001–0.02 M¤? IR dust observations: only ~10 SNe + SNRs e.g. Sugerman et al. (2006), Matsuura et al. (2015), De Looze et al. (2017; 2019) Target opportunity – extra-galactic SNe SN 2014J 2MASS pre-explosion SOFIA/FLITECAM SOFIA observations of SN 2014J in M82 – unfortunately no dust Template for extragalactic SNe – Time evolution of SN 1987A SOFIA SN 1987A (50kpc) • The peak of SED shifted to longer wavelength in tiMe • The inferred mass increases in tiMe? • 0.001 M¤ at day 615 Harvey et al. (1989), Wooden et al.
    [Show full text]
  • 1. Basic Properties of Supernovae During the Past Two Decades, There Has Occurred a Technological Break-Through in Astronomy
    PHYSICS of SUPERNOVAE: THEORY, OBSERVATIONS, UNRESOLVED PROBLEMS * D. K. Nadyozhin Institute for Theoretical and Experimental Physics, Moscow. [email protected] The main observational properties and resulting classification of supernovae (SNe) are briefly reviewed. Then we discuss the progress in modeling of two basic types of SNe – the thermonuclear and core-collapse ones, with special emphasis being placed on difficulties relating to a consistent description of thermonuclear flame propagation and the detachment of supernova envelope from the collapsing core (a nascent neutron star). The properties of the neutrino flux expected from the core- collapse SNe, and the lessons of SN1987A, exploded in the Large Magellanic Cloud, are considered as well. 1. Basic Properties of Supernovae During the past two decades, there has occurred a technological break-through in astronomy. The sensitivity, spectral and angular resolution of detectors in the whole electromagnetic diapason from gamma-rays through radio wavelengths has been considerably increased. Hence, it became possible to derive from the observed supernova spectra precise data on dynamics of supernova expansion and on composition and light curves of SNe as well. Moreover, neutrino astronomy overstepped the bounds of our Galaxy to discover the neutrino signal from SN1987A. This epoch- making event had a strong impact on the theory of supernovae. The main indicator for supernova astronomical classification is the amount of hydrogen observed in the SN envelopes. The Type I SNe (subtypes Ia, Ib, Ic) contain no hydrogen in their envelopes. The SN Ia are distinguished by strong Si lines in their spectra and form quite a homogeneous group of objects. On the contrary, Type II SNe (subtypes IIP, IIn, IIL, IIb) have clear lines of hydrogen in their spectra (Fig.
    [Show full text]
  • Pos(GOLDEN2019)046 Model 6 Model May Be Inconsistent 6 Model Can Be Also Progenitors of Peculiar Sne Ia
    Progenitor and explosion models of type Ia supernovae PoS(GOLDEN2019)046 Ataru Tanikawa∗ Department of Earth Science and Astronomy, College of Arts and Sciences, The University of Tokyo, 3-8-1 Komaba, Meguro-ku, Tokyo 153-8902, Japan E-mail: [email protected] Type Ia supernovae (SNe Ia) are important objects in astronomy and astrophysics. They are one of the brightest and common transients in the universe, a standard candle for a cosmic distance, and a dominant origin of iron group elements. It is widely accepted that SNe Ia are thermodynamical explosions of carbon-oxygen (CO) white dwarfs (WDs) in binary systems. Nevertheless, it is yet unclear what the companion stars are, and what the masses of the exploding CO WDs are. Recently, many sub-Chandrasekhar mass explosions in the double-degenerate scenario have been suggested. We have assessed the violent merger and Dynamically-Driven Double-Degenerate Double-Detonation (D6) models by numerical simulations. We have concluded that the violent merger model may not explain normal SNe Ia, since their circum-binary matter is much larger than the size of SN 2011fe, and their event rate is much smaller than the SN Ia rate in our Galaxy by an order of magnitude. However, it can be progenitors of peculiar SNe Ia. The D6 model has roughly consistent features with normal SNe Ia. However, the model has supernova ejecta with an asymmetric shape and low-velocity carbon-oxygen component due to the presence of the surviving companion CO. If these features can be observed, the D6 model may be inconsistent with normal SNe Ia.
    [Show full text]